dc.contributor | Universidade Estadual Paulista (Unesp) | |
dc.date.accessioned | 2013-09-30T18:53:41Z | |
dc.date.accessioned | 2014-05-20T14:09:32Z | |
dc.date.accessioned | 2022-10-05T15:05:19Z | |
dc.date.available | 2013-09-30T18:53:41Z | |
dc.date.available | 2014-05-20T14:09:32Z | |
dc.date.available | 2022-10-05T15:05:19Z | |
dc.date.created | 2013-09-30T18:53:41Z | |
dc.date.created | 2014-05-20T14:09:32Z | |
dc.date.issued | 2010-04-01 | |
dc.identifier | Journal of High Energy Physics. New York: Springer, n. 4, p. 13, 2010. | |
dc.identifier | 1126-6708 | |
dc.identifier | http://hdl.handle.net/11449/24184 | |
dc.identifier | 10.1007/JHEP04(2010)067 | |
dc.identifier | WOS:000277473100003 | |
dc.identifier.uri | http://repositorioslatinoamericanos.uchile.cl/handle/2250/3897381 | |
dc.description.abstract | Four-dimensional super-twistors provide a compact covariant description of on-shell N = 4 d=4 super-Yang-Mills. In this paper, ten-dimensional super-twistors are introduced which similarly provide a compact covariant description of on-shell d=10 super-Yang-Mills. The super-twistor variables are Z - (lambda(alpha), mu(alpha), Gamma(m)) where lambda(alpha) and mu(alpha) are constrained bosonic d=10 spinors and Gamma(m) is a constrained fermionic d=10 vector. The Penrose map relates the twistor superfield Phi(Z) with the d=10 super-Yang-Mills vertex operator lambda(alpha) A(alpha)(x,theta) which appears in the pure spinor formalism of the superstring, and the cubic super-Yang-Mills amplitude is proportional to the super- twistor integral f dZ Phi(1)Phi(2)Phi(3). | |
dc.language | eng | |
dc.publisher | Springer | |
dc.relation | Journal of High Energy Physics | |
dc.relation | 1,227 | |
dc.rights | Acesso restrito | |
dc.source | Web of Science | |
dc.subject | Superspaces | |
dc.subject | Field Theories in Higher Dimensions | |
dc.title | Ten-dimensional super-twistors and Super-Yang-Mills | |
dc.type | Artigo | |